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Production of  Mesons on Protons near Threshold by Linearly Polarized Photon at SPring-8/LEPS

PaNic02. XVI Particles and Nuclei International Conference September 30 - October 4, 2002, Osaka, Japan. Production of  Mesons on Protons near Threshold by Linearly Polarized Photon at SPring-8/LEPS. Wen-Chen Chang for LEPS collaboration

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Production of  Mesons on Protons near Threshold by Linearly Polarized Photon at SPring-8/LEPS

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  1. PaNic02 XVI Particles and Nuclei International Conference September 30 - October 4, 2002, Osaka, Japan Production of  Mesons on Protons near Threshold by Linearly Polarized Photon at SPring-8/LEPS Wen-Chen Chang for LEPS collaboration Institute of Physics, Academia Sinica Taipei 11529, Taiwan

  2. Outline • Photo-production of  mesons at high energy and near production threshold. • Pomeron exchange. • Pseduo-scaler particle exchange. • How linearly polarized photon beam can help us in distinguishing different sources of contribution? • Spin density matrix element. • Decay asymmetry in Helicity Frame. • Measurement by LEPS experiment at SPring-8. • Reconstruction of  mesons in KK modes. • Angular distribution of K+ in Helicity Frame at forward direction. • Summary.

  3. Total Cross Section of Hadronic Interaction A. Donnachie and P.V. Landshoff Universal Scaling : = 0.5,  = 0.08

  4. (OZI Suppressed!) Pseudo-scaler Exchange Exotic knock-out process Photo-Production of  Mesonsat Forward Region (small |t|) Pomeron Exchange

  5. Photo-Production of  Mesonsat Backward region (large |t|)  Emission from Nucleon Exotic shake-off process

  6. At Forward region: • Pomeron: • Positive power-law scaling of s. • Dominating at large energy. • Natural parity (=+1). • Exchange particles unknown; likely to be glueball : P1(J=2+), P2(J=0+, negative power-law scaling of s). (Ref. T. Nakano and H.Toki, 1998) • Successful phenomenology for diffractive process. • Pseudo-scaler particle: • Negative power-law scaling of s. • Showing up at small energy. • Un-natural parity (= –1). • Exchange particles like ,. • OZI suppressed.

  7. Differential Cross section of p   p with un-polarized photon beams (t=0) A.I.Titov et. al., PRC 59, R2993

  8. With Linearly-Polarized Photon Beam • Experimentally we measure W’s functions and density matrix  could be determined by spherical harmonics decomposition. • The contributions of natural and un-natural parity exchange in the t-channel are represented by the matrix element of Re(0), Re(1).  H: polar angle of K+ in Helicity frame  H : azimuthal angle of K+ in Helicity frame : angle between the photon polarization vector and CMS production plane.

  9. Spin Density Matrix Elements K.Schilling et. al., Nucl. Phys. B15 (1970) 397

  10. The Spin Density Matrix Elements at small |t| regions • Two important spin-conserving processes: • Pomeron exchange: 11-1= –Im 21-1 = +0.5, and all diagonal ’s = 0 at =0. • , exchange: 11-1= –Im 21-1 = – 0.5, and all diagonal ’s = 0 at =0. A.I.Titov et. al., PRC60, 035205

  11. Angular Distribution of K+ in Helicity Frame =0, 11-1=+0.5 =1, 11-1= – 0.5

  12. SLAC MeasurementJ.Ballam, et. al, PRD 7(1973), 3150

  13. RCNP, Osaka University, Japan H. Fujimura, M. Fujiwara, T. Hotta, H. Kohri, T. Matsumura, N. Matsuoka, T. Mibe, M. Morita, T.Nakano, T. Yorita Osaka University, Japan N. Nomachi, A. Sakaguchi, Y. Sugaya, M. Sumihama Academia Sinica, Taiwan W.C. Chang, D.S. Oshuev, C.W. Wang, S.C. Wang Chiba University, Japan H. Kawai, T. Ooba, Y. Shiino IHEP, Russia P. Shagin JAERI, Japan Y. Asano, N. Muramatsu, R.G.T. Zegers JASRI, Japan S. Date, N. Kumagai, Y. Ohashi, H. Ookuma Konan University, Japan H. Akimune Kyoto University, Japan K. Imai, T. Ishikawa, M.Miyabe, M.Niiyamma ,M. Yosoi Nagoya University, Japan S. Fukui, T. Iwata, Y. Miyachi, A. Wakai Ohio University, U.S. K. Hicks Pusan National University, S. Korea J.K. Ahn Saskatchewan University, Canada C. Rangacharyulu Tohoku University, Japan H. Shimizu Wakayam Med. University, Japan S. Makino LEPS Collaboration

  14. g LEPS detectors Dipole Magnet (0.7 T) TOF wall Start counter Liquid Hydrogen Target 50mm-long (2000 Dec.-2001June) 150mm-long (2002May-July) Aerogel Cerenkov (n=1.03) MWDC 3 Silicon Vertex Detector MWDC 2 MWDC 1 1m

  15. K/p separation (positive charge) Reconstructed mass p- p+ p+ p K+ K+ Events d Momentum (GeV) K- Mass(GeV) Mass/Charge (GeV) Charged particle identification

  16. Signal of   K+K

  17. Reconstructed fevents • Large acceptance at forward angles • ~5000 f’s (Dec,2000 - June, 2001) • Runs with 150mm-long LH2 target (May-July, 2002 ). KK event Kp event

  18. Experimental Acceptance at-0.2< t < |t|min GeV2 2.2 < Eg < 2.4 GeV

  19. Simulation at-0.2< t < |t|min GeV2 2.2 < Eg < 2.4 GeV =0 =0.5 =1

  20. |M(KK)-Mf |< 10 MeV , |M((KK)X)-Mproton|< 30 MeV -0.2< t < |t|min GeV2 , 2.2 < Eg < 2.4 GeV w/o Acceptance Correction Decay angular distribution of K+in f rest frame (Helicity frame) Horizontally polarized beam Vertically polarized beam Raw Data

  21. Summary • About 5000 events of photo-production of  mesons by linearly polarized photons from Eg= 1.6GeV(threshold) to 2.4GeV are measured by LEPS experiment at SPring-8/Japan. • In comparison with measurement at high energy, our preliminary results show that the contribution of natural-parity exchange still composes a larger fraction in the total scattering amplitude while that of un-natural parity component becomes more significant at E=2.3 GeV and t>-0.2 region. • With the ongoing studies of the acceptance correction and systematic errors, the cross section, differential cross section and spin density matrix elements at the forward regions will be reported in the near future. A presentation of detailed results will be shown in the poster session: “Polarization observables in the \phi(1020) meson photoproduction with linearly polarized photons” by T. Mibe (RCNP, Osaka Univ.).

  22. Decay Angular Distribution in  p   p

  23. Example

  24. Super Photon Ring 8 GeV (SPring-8)

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